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Crystallization Mechanism in Spark Plasma Sintered Bulk Metallic Glass Analyzed using Small Angle Neutron Scattering

Understanding the thermal stability of metallic glasses is critical to determining their safe temperatures of service. In this paper, the crystallization mechanism in spark plasma sintered Fe(48)Cr(15)Mo(14)Y(2)C(15)B(6) metallic glass is established by analyzing the crystal size distribution using...

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Autores principales: Paul, Tanaji, Singh, Ashish, Littrell, Kenneth C., Ilavsky, Jan, Harimkar, Sandip P.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group UK 2020
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7005171/
https://www.ncbi.nlm.nih.gov/pubmed/32029831
http://dx.doi.org/10.1038/s41598-020-58748-3
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author Paul, Tanaji
Singh, Ashish
Littrell, Kenneth C.
Ilavsky, Jan
Harimkar, Sandip P.
author_facet Paul, Tanaji
Singh, Ashish
Littrell, Kenneth C.
Ilavsky, Jan
Harimkar, Sandip P.
author_sort Paul, Tanaji
collection PubMed
description Understanding the thermal stability of metallic glasses is critical to determining their safe temperatures of service. In this paper, the crystallization mechanism in spark plasma sintered Fe(48)Cr(15)Mo(14)Y(2)C(15)B(6) metallic glass is established by analyzing the crystal size distribution using x-ray diffraction, transmission electron microscopy and in-situ small angle neutron scattering. Isothermal annealing at 700 °C and 725 °C for 100 min resulted in the formation of (Fe,Cr)(23)C(6) crystals, measured from transmission electron micrographs, to be from 10 to 30 nm. The small angle neutron scattering intensity measured in-situ, over a Q-range of 0.02 to 0.3 Å(−1), during isothermal annealing of the sintered samples, confirmed the presence of (Fe,Cr)(23)C(6) crystals. The measured scattering intensity, fitted by the maximum entropy model, over the Q-range of 0.02 to 0.06 Å(−1), revealed that the crystals had radii ranging from 3 to 18 nm. The total volume fraction of crystals were estimated to be 0.13 and 0.22 upon isothermal annealing at 700 °C and 725 °C for 100 min respectively. The mechanism of crystallization in this spark plasma sintered iron based metallic glass was established to be from pre-existing nuclei as confirmed by Avrami exponents of 0.25 ± 0.01 and 0.39 ± 0.01 at the aforesaid temperatures.
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spelling pubmed-70051712020-02-18 Crystallization Mechanism in Spark Plasma Sintered Bulk Metallic Glass Analyzed using Small Angle Neutron Scattering Paul, Tanaji Singh, Ashish Littrell, Kenneth C. Ilavsky, Jan Harimkar, Sandip P. Sci Rep Article Understanding the thermal stability of metallic glasses is critical to determining their safe temperatures of service. In this paper, the crystallization mechanism in spark plasma sintered Fe(48)Cr(15)Mo(14)Y(2)C(15)B(6) metallic glass is established by analyzing the crystal size distribution using x-ray diffraction, transmission electron microscopy and in-situ small angle neutron scattering. Isothermal annealing at 700 °C and 725 °C for 100 min resulted in the formation of (Fe,Cr)(23)C(6) crystals, measured from transmission electron micrographs, to be from 10 to 30 nm. The small angle neutron scattering intensity measured in-situ, over a Q-range of 0.02 to 0.3 Å(−1), during isothermal annealing of the sintered samples, confirmed the presence of (Fe,Cr)(23)C(6) crystals. The measured scattering intensity, fitted by the maximum entropy model, over the Q-range of 0.02 to 0.06 Å(−1), revealed that the crystals had radii ranging from 3 to 18 nm. The total volume fraction of crystals were estimated to be 0.13 and 0.22 upon isothermal annealing at 700 °C and 725 °C for 100 min respectively. The mechanism of crystallization in this spark plasma sintered iron based metallic glass was established to be from pre-existing nuclei as confirmed by Avrami exponents of 0.25 ± 0.01 and 0.39 ± 0.01 at the aforesaid temperatures. Nature Publishing Group UK 2020-02-06 /pmc/articles/PMC7005171/ /pubmed/32029831 http://dx.doi.org/10.1038/s41598-020-58748-3 Text en © UChicago Argonne, LLC, UT-Battelle and the Author(s) 2020 Open Access This article is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made. The images or other third party material in this article are included in the article’s Creative Commons license, unless indicated otherwise in a credit line to the material. If material is not included in the article’s Creative Commons license and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this license, visit http://creativecommons.org/licenses/by/4.0/.
spellingShingle Article
Paul, Tanaji
Singh, Ashish
Littrell, Kenneth C.
Ilavsky, Jan
Harimkar, Sandip P.
Crystallization Mechanism in Spark Plasma Sintered Bulk Metallic Glass Analyzed using Small Angle Neutron Scattering
title Crystallization Mechanism in Spark Plasma Sintered Bulk Metallic Glass Analyzed using Small Angle Neutron Scattering
title_full Crystallization Mechanism in Spark Plasma Sintered Bulk Metallic Glass Analyzed using Small Angle Neutron Scattering
title_fullStr Crystallization Mechanism in Spark Plasma Sintered Bulk Metallic Glass Analyzed using Small Angle Neutron Scattering
title_full_unstemmed Crystallization Mechanism in Spark Plasma Sintered Bulk Metallic Glass Analyzed using Small Angle Neutron Scattering
title_short Crystallization Mechanism in Spark Plasma Sintered Bulk Metallic Glass Analyzed using Small Angle Neutron Scattering
title_sort crystallization mechanism in spark plasma sintered bulk metallic glass analyzed using small angle neutron scattering
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7005171/
https://www.ncbi.nlm.nih.gov/pubmed/32029831
http://dx.doi.org/10.1038/s41598-020-58748-3
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